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examples
extended
electromagnetic
TestEm7
include
G4LindhardPartition.hh
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//
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// ********************************************************************
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// * License and Disclaimer *
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// * *
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// * The Geant4 software is copyright of the Copyright Holders of *
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// * the Geant4 Collaboration. It is provided under the terms and *
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// * conditions of the Geant4 Software License, included in the file *
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// * LICENSE and available at http://cern.ch/geant4/license . These *
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// * include a list of copyright holders. *
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// * *
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// * Neither the authors of this software system, nor their employing *
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// * institutes,nor the agencies providing financial support for this *
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// * work make any representation or warranty, express or implied, *
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// * regarding this software system or assume any liability for its *
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// * use. Please see the license in the file LICENSE and URL above *
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// * for the full disclaimer and the limitation of liability. *
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// * *
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// * This code implementation is the result of the scientific and *
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// * technical work of the GEANT4 collaboration. *
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// * By using, copying, modifying or distributing the software (or *
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// * any work based on the software) you agree to acknowledge its *
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// * use in resulting scientific publications, and indicate your *
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// * acceptance of all terms of the Geant4 Software license. *
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// ********************************************************************
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//
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/*
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* \file electromagnetic/TestEm7/include/G4LindhardPartition.hh
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* \brief Definition of the G4LindhardPartition class
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*
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* Created by Marcus Mendenhall on 1/14/08.
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* 2008 Vanderbilt University, Nashville, TN, USA.
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*
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*/
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// $Id: G4LindhardPartition.hh 66586 2012-12-21 10:48:39Z ihrivnac $
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//
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#include "
globals.hh
"
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class
G4Material
;
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class
G4VNIELPartition
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{
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public
:
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G4VNIELPartition
() { }
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virtual
~G4VNIELPartition
() { }
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// return the fraction of the specified energy which will be deposited as NIEL
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// if an incoming particle with z1, a1 is stopped in the specified material
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// a1 is in atomic mass units, energy in native G4 energy units.
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virtual
G4double
PartitionNIEL
(
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G4int
z1,
G4double
a1,
const
G4Material
*material,
G4double
energy
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)
const
=0;
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};
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class
G4LindhardRobinsonPartition
:
public
G4VNIELPartition
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{
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public
:
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G4LindhardRobinsonPartition
();
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virtual
~G4LindhardRobinsonPartition
() { }
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virtual
G4double
PartitionNIEL
(
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G4int
z1,
G4double
a1,
const
G4Material
*material,
G4double
energy
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)
const
;
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G4double
z23
[120];
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size_t
max_z
;
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};
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G4LindhardRobinsonPartition::max_z
size_t max_z
Definition:
G4LindhardPartition.hh:67
G4Material
Definition:
G4Material.hh:121
G4LindhardRobinsonPartition::z23
G4double z23[120]
Definition:
G4LindhardPartition.hh:66
G4LindhardRobinsonPartition::~G4LindhardRobinsonPartition
virtual ~G4LindhardRobinsonPartition()
Definition:
G4LindhardPartition.hh:60
G4double
double G4double
Definition:
G4Types.hh:76
energy
double energy
Definition:
plottest35.C:25
G4VNIELPartition::G4VNIELPartition
G4VNIELPartition()
Definition:
G4LindhardPartition.hh:45
G4VNIELPartition::PartitionNIEL
virtual G4double PartitionNIEL(G4int z1, G4double a1, const G4Material *material, G4double energy) const =0
globals.hh
G4LindhardRobinsonPartition::G4LindhardRobinsonPartition
G4LindhardRobinsonPartition()
Definition:
G4LindhardPartition.cc:66
G4LindhardRobinsonPartition::PartitionNIEL
virtual G4double PartitionNIEL(G4int z1, G4double a1, const G4Material *material, G4double energy) const
Definition:
G4LindhardPartition.cc:72
G4int
int G4int
Definition:
G4Types.hh:78
G4VNIELPartition::~G4VNIELPartition
virtual ~G4VNIELPartition()
Definition:
G4LindhardPartition.hh:46
G4VNIELPartition
Definition:
G4LindhardPartition.hh:42
G4LindhardRobinsonPartition
Definition:
G4LindhardPartition.hh:56
다음에 의해 생성됨 :
1.8.5